Related Experiment Video
Updated: Jul 10, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Universal Scaling near Band-Tuned Metal-Insulator Phase Transitions
Simone Fratini1, Sergio Ciuchi2,3, Vladimir Dobrosavljević4
1Université Grenoble Alpes, CNRS, Grenoble INP, Institut Néel, 38000 Grenoble, France.
We developed a theory explaining metal-insulator transitions, revealing scaling behaviors and a "fake insulator" regime. This framework clarifies observations in various materials, including high-temperature metals with negative resistivity changes.
Area of Science:
- Condensed Matter Physics
- Materials Science
Background:
- Metal-insulator transitions are crucial phenomena in condensed matter.
- Understanding the behavior of resistivity near these transitions is key.
- Existing theories struggle to explain certain experimental observations like negative dR/dT.
Purpose of the Study:
- To present a theoretical framework for band-tuned metal-insulator transitions.
- To explain the scaling of resistivity curves and the "fake insulator" regime.
- To reconcile Mooij correlations in high-temperature metals with theoretical predictions.
Main Methods:
- Utilizing the Kubo formalism for theoretical analysis.
- Investigating scaling behaviors in resistivity under specific conditions (Tτ>1 or μτ>1).
- Analyzing the power-law divergence of resistivity at critical chemical potential.
Main Results:
- The theory predicts resistivity scaling in a specific regime.
- A power-law divergence of resistivity (R_{c}∼1/T) at the critical chemical potential.
- Identification of a "fake insulator" regime with negative dR/dT on the metallic side, explaining experimental findings.
Conclusions:
- The proposed theory successfully explains scaling and the "fake insulator" phenomenon.
- This framework quantitatively accounts for Mooij correlations in high-temperature metals.
- The theory provides a unified understanding of metal-insulator transitions across diverse experimental systems.
More Related Videos
Related Concept Videos
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Band Theory
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
Scaling
Theory of Metallic Conduction
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
Semiconductors
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...

